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Code Manual for CONTAIN 2.0 - Federation of American Scientists

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—<br />

For any sectional coefficient ~, the interpolated sectional coefficients are given by<br />

g = (1 - FT)[(l -FP)~ll + FP512 ] + %[(1 -FP)321 + FP522] (7-5)<br />

where I& is the aerosol coefilcient <strong>for</strong> some process <strong>for</strong> the lowest atmospheric temperature (Tti~)<br />

and pressure (P~i~),~12 is the aerosol coefficient <strong>for</strong> that process <strong>for</strong> the 10west atrnosPheric<br />

temperature (T~i~)and highest pressure (p~m), (~21) is tie aerosol <strong>for</strong> the ~ghest atmospheric<br />

temperature (T~m) and lowest pressure (pW,), ~d ~zz is the aerosol coefficient <strong>for</strong> the ~ghest<br />

atmospheric temperature (T~M)and pressure (P~u).<br />

F~ and FPin Equation (7-5) are defined as<br />

and<br />

Fp =<br />

[)<br />

Pg - Ptin<br />

P “ Pfin<br />

max<br />

where T~is the atmosphere temperature, and P~is the atmosphere pressure.<br />

It should be noted that not all aerosol modeling is cast in coefficient <strong>for</strong>m, because <strong>of</strong> the limitations<br />

discussed above. In particular, coefficients are not used <strong>for</strong> the aerosol deposition models <strong>for</strong><br />

engineered systems, which are discussed in Sections 7.4 through 7.6, or <strong>for</strong> the moving grid<br />

condensation model. With regard to engineered systems, the full expressions <strong>for</strong> the deposition rates<br />

are always used and properly evaluated with respect to local boundag layer conditions. The<br />

deposition rate, however, is evaluated only <strong>for</strong> one representative particle diameter within each<br />

section, taken to be the geometric mean <strong>of</strong> the upper and lower diameters in the section. This<br />

approach is believed to be adequate. With regard to the moving grid model, the effects <strong>of</strong><br />

condensation or evaporation are evaluated by calculating the change in particle size with time, then<br />

redistributing the time-evolved distribution into the fixed sections. The effects cannot be represented<br />

in terms <strong>of</strong> the time-independent ~ coel%cients shown in Equation (7-3).<br />

In the following discussion, <strong>for</strong> simplicity, only the discrete <strong>for</strong>ms <strong>of</strong> the agglomeration kernels and<br />

deposition rate equations will be presented. The approximations inherent in the use <strong>of</strong> the coefficient<br />

approach, if applicable, will be indicated.<br />

7.2.1 Agglomeration<br />

When two aerosol particles collide, they can combine to <strong>for</strong>m a larger particle. This process is<br />

known as agglomeration or coagulation. A basic assumption about these processes is that only two<br />

Rev O 711 6/30/97

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